Optical Information Recording Method, Optical Information Recording Apparatus, and Optical Information Recording Medium

ABSTRACT

It is an object to be able to record data with good signal quality over a wide range of linear velocities to an optical information recording medium. To achieve the stated object, in a laser drive circuit ( 5 ) of an optical information recording apparatus, the ratio of recording power to the power at which the reproduction signal quality reaches a threshold value is set to be relatively low at low velocities, and relatively high at high velocities.

TECHNICAL FIELD

The present invention relates to an optical information recording methodfor recording to an optical information recording medium with which datais optically recorded and reproduced, and to an apparatus for recordingthe same, and a recording medium, and more particularly relates to amethod for recording to an optical information recording medium withwhich information is recorded at a plurality of different linearvelocities.

BACKGROUND ART

Optical disks, optical cards, optical tapes, and so forth have beenproposed and developed in recent years as media for optically recordingdata. Optical disks have become especially popular as media that allowlarge volumes of data to be recorded and reproduced at high density.

For instance, in the case of a phase-change optical disk, data isrecorded and reproduced by the following method. The recording film ofan optical disk is irradiated with a laser beam focused by an opticalhead and stronger in power than the reproduction power (this power levelwill be referred to as the recording power, and expressed as Pp), andwhen the temperature of the recording film goes over the melting point,the molten portion is rapidly cooled as the laser beam is transmitted,and this forms a mark in an amorphous state. When the recording film isirradiated with a laser beam that has been focused enough to raise thetemperature of the recording film to at least its crystallizationtemperature but below its melting point (this power level will bereferred to as the erasure power, and expressed by Pb), the irradiatedportion of the recording film enters a crystalline state. As a result, arecorded pattern consisting of marks (amorphous regions) and spaces(crystalline regions) corresponding to a data signal is formed on theoptical disk. The data is then reproduced by taking advantage of thedifference in reflectance between the crystalline and amorphous regions.

As described above, to form marks on a medium, it is necessary tomodulate the power level of the emitted laser beam at least betweenerasure power and recording power. The pulse waveform used in themodulation operation is called a recording pulse. Many recording methodsfor forming a single mark with a plurality of recording pulses havealready been disclosed. The plurality of recording pulses is called arecording pulse train. FIG. 10 a shows an example of a recording pulsetrain. A pulse at the front part of the recording pulse train is calledthe leading pulse 501, a pulse at the end of the recording pulse trainis referred to as the trailing pulse 503, and a pulse between theleading pulse 501 and the trailing pulse 503 is called a multi-pulse502. The number of recording pulses that make up the recording pulsetrain varies with the recording code length (that is, the length of therecording code with respect to a channel clock period Tw), and at theshortest code length, there may be only one recording pulse. Theintensity of the laser beam is modulated as shown in FIG. 10 b on thebasis of this recording pulse train. As a result, a mark 302 is formedon a track 301 as shown in FIG. 10 c. A method in which a mark is formedby using a laser irradiation waveform in which the pulse level is variedbetween the leading portion and the trailing portion as shown in FIG.11, instead of using a recording pulse train, has also been disclosed.

At present, DVDs and other such optical information recording mediaprimarily make use of constant linear velocity (CLV) recording. This isa system for recording data at substantially the same linear velocity,transfer rate, and linear density over the entire surface of the medium.An advantage therefore is that there is no change in the laser beamirradiation conditions or in heating/cooling conditions during recordingand reproduction. On the other hand, since the rotational speed of themedium varies with the recording or reproduction position (that is, theradial position) on the medium, controlling the rotational speed changesof a spindle motor is essential.

In contrast, a constant angular velocity (CAV) recording system, inwhich the rotational speed and the linear density of the medium are keptsubstantially constant over the entire surface of the medium, has beenproposed. Unlike with a CLV recording system, a CAV recording systemdoes not require control of the rotational speed changes of a spindlemotor for rotating the medium, so an advantage is that the spindle motorand the control circuit thereof can be produced at lower cost. Also,there is no need to wait for a recording or reproduction operation untila specific rotational speed is attained after seeking the recording orreproduction position, so the access speed with respect to the mediumcan be shortened. On the other hand, a CAV recording system, the linearvelocity and the transfer rate of the medium vary with the recording orreproduction position in the medium. Therefore, the conditions underwhich the medium is irradiated with the laser beam, and theheating/cooling conditions vary with the recording or reproductionposition.

Improving recorded signal quality in either of these systems isimportant in terms of recording or reproducing large volumes of data athigh density. Accordingly, methods have already been disclosed forimproving signal quality by adjusting the recording power with respectto a certain linear velocity (the recording or reproduction position inthe case of CAV recording). One such method that has been disclosedinvolves recording a test signal while the recording power or erasurepower is varied, and determining the power levels on the basis of therecorded test signal so that the asymmetry or degree of modulation ofthe reproduction signal is optimized (see Patent Document 1, forexample).

However, with the above-mentioned conventional recording method, if thelinear velocity is varied over a large range in CAV recording, theoptimal conditions will be different for each linear velocity, so a datasignal cannot be recorded stably and with good signal quality. Thisproblem will now be described.

During recording at a high linear velocity, the spindle motor rotates athigh speed. Consequently, if there is even a slight axial runout oreccentricity to the disk, this will have a major impact on servooperation. Specifically, if there is axial runout in the disk, theactuator of the optical head will oscillate strongly in the optical axisdirection. If there is eccentricity in the disk, the actuator willoscillate strongly in the direction parallel to the plane of the disk.If this oscillation exceeds the response characteristics of theactuator, the actuator will be unable to keep up with the axial runoutor eccentricity of the disk, defocusing or off-tracking will occur, andthe signal cannot be recorded stably.

On the other hand, during recording at a low linear velocity, therelative speed between the laser spot and the medium is lower, andcooling after melting caused by laser irradiation is slower, sorecrystallization proceeds from the edges of the molten part, and theremaining portion becomes a mark. Accordingly, as shown in FIG. 12, amolten region 303 is larger than a mark 302, and the end of the moltenregion extends all the way to the walls 304 of a track 301 (that is, aguide groove or land). As a result, this affects the fine shape of thewalls 304 (causing looseness), recrystallization does not occur in partof the molten region reaching the walls 304, and parts of the mark stickto the walls 304. Consequently, the shape of the mark is distorted andthis lowers the quality of the reproduction signal.

Patent Document 1: Japanese Unexamined Patent Publication No. H10-64064

DISCLOSURE OF THE INVENTION

It is an object of the present invention to solve the above-mentionedproblems encountered in the past, and to provide an optical informationrecording method, an optical information recording apparatus, and anoptical information recording medium with which data can be recorded toand reproduced from a given medium at stable and good signal qualityover a wide range of linear velocities.

To achieve the stated object, the present invention is an opticalinformation recording method, comprising, irradiating an opticalinformation recording medium with a laser beam, forming marks or spacesso that the optical characteristics of a recording film are varied,forming the marks by recording pulses or a recording pulse train inwhich the power of the laser beam is switched between a plurality ofpower levels including at least a recording power and erasure power, andrecording information at two different linear velocities, wherein therecording power is controlled so as to satisfy (Pp1/Ppth1)<(Pp2/Ppth2),where Ppth1 is the threshold value of the recording power at which thequality of a reproduction signal drops under a specific value when atest signal is recorded at a first linear velocity v1 with the erasurepower fixed and the recording power varied, Ppth2 is the threshold valueof the recording power at which the quality of the reproduction signaldrops under a specific value when the test signal is recorded at asecond linear velocity v2 that is higher than the first linear velocityv1, with the erasure power fixed and the recording power varied, Pp1 isthe recording power when the information is recorded at the first linearvelocity v1, and Pp2 is the recording power when the information isrecorded at the second linear velocity v2.

With this method, a mark can be formed with no distortion at low linearvelocities, and a satisfactory power margin can be ensured in recordingat high linear velocities, so data can be recorded at good signalquality over a wider range of linear velocities.

In the above invention, the criterion for the quality of thereproduction signal may be the jitter of the reproduction signal.

In the above invention, the criterion for the quality of thereproduction signal may be a value based on the error rate of thereproduction signal.

In the above invention, the criterion for the quality of thereproduction signal may be a value based on the degree of modulation ofthe reproduction signal.

In all of the above cases, it is possible to record data at good signalquality.

The present invention is also an optical information recording method,comprising, irradiating an optical information recording medium with alaser beam, forming marks or spaces so that the optical characteristicsof a recording film are varied, forming the marks by recording pulses ora recording pulse train in which the power of the laser beam is switchedbetween a plurality of power levels including at least a recording powerand erasure power, and recording information at two different linearvelocities, wherein the recording power is controlled so as to satisfy(Pp1/Ppth1)<(Pp2/Ppth2), where Ppth1 is the threshold value of therecording power at which the quality of a reproduction signal dropsunder a specific value when a test signal is recorded at a first linearvelocity v1, with the erasure power and the recording power varied suchthat the ratio between these powers is constant, Ppth2 is the thresholdvalue of the recording power at which the quality of the reproductionsignal drops under a specific value when the test signal is recorded ata second linear velocity v2 that is higher than the first linearvelocity v1, with the erasure power and the recording power varied suchthat the ratio between these powers is constant, Pp1 is the recordingpower when the information is recorded at the first linear velocity v1,and Pp2 is the recording power when the information is recorded at thesecond linear velocity v2.

Again with this method, a mark can be formed with no distortion at lowlinear velocities, and a satisfactory power margin can be ensured inrecording at high linear velocities, so data can be recorded at goodsignal quality over a wider range of linear velocities.

The present invention is also an optical information recording method,comprising, irradiating an optical information recording medium with alaser beam, forming marks or spaces so that the optical characteristicsof a recording film are varied, forming the marks by recording pulses ora recording pulse train in which the power of the laser beam is switchedbetween a plurality of power levels including at least a recording powerand erasure power, and recording information at two different linearvelocities, wherein the recording power is controlled so as to satisfya1<a2, where a1 is the asymmetry of the reproduction signal when a testsignal is recorded at a first linear velocity v1, with the erasure powerfixed and the recording power varied, and a2 is the asymmetry of thereproduction signal when the test signal is recorded at a second linearvelocity v2 that is higher than the first linear velocity v1, with theerasure power fixed and the recording power varied.

The present invention is also an optical information recording method,comprising, irradiating an optical information recording medium with alaser beam, forming marks or spaces so that the optical characteristicsof a recording film are varied, forming the marks by recording pulses ora recording pulse train in which the power of the laser beam is switchedbetween a plurality of power levels including at least a recording powerand erasure power, and recording information at two different linearvelocities, wherein the recording power is controlled so as to satisfya1<a2, where a1 is the asymmetry of the reproduction signal when a testsignal is recorded at a first linear velocity v1, with the erasure powerand the recording power varied such that the ratio between these powersis constant, and a2 is the asymmetry of the reproduction signal when thetest signal is recorded at a second linear velocity v2 that is higherthan the first linear velocity v1, with the erasure power and therecording power varied such that the ratio between these powers isconstant.

Again with these methods, a mark can be formed with no distortion at lowlinear velocities, and a satisfactory power margin can be ensured inrecording at high linear velocities, so data can be recorded at goodsignal quality over a wider range of linear velocities.

The optical information recording method of the present invention ischaracterized in that the recording system is a CAV recording system.

With this method, data can be recorded at good signal quality regardlessof where the recording or reproduction position is in the medium.

The optical information recording method of the present invention ischaracterized in that the recording power is controlled so that Pp isincreased according to the increase in a linear velocity v when Pp isthe recording power at the linear velocity v, which is a value betweenthe first linear velocity v1 and the second linear velocity v2.

With this method, the recording power can be easily determined at anintermediate linear velocity.

The optical information recording method of the present invention ischaracterized in that the power level between recording pulses iscontrolled to be different from the erasure power.

Also, the optical information recording method of the present inventionis characterized in that the power coefficient between recording pulsesat the second linear velocity v2 is controlled to be higher than thepower coefficient between recording pulses at the first linear velocityv1 when the power coefficient between recording pulses is α andα=(Pbtm−Pb)/(Pp−Pb), where Pp is the recording power, Pb is the erasurepower, and Pbtm is the power level between recording pulses.

With this method, the cooling rate during recording can be optimallycontrolled according to the linear velocity, which means that data canbe recorded at good signal quality.

To achieve the stated object, the optical information recording mediumof the present invention is characterized in that information expressingthe value of Pp1/Ppth1 and Pp2/Ppth2 is recorded.

Also, the optical information recording medium of the present inventionis characterized in that information expressing the value of Pp1 and Pp2is recorded.

Also, the optical information recording medium of the present inventionis characterized in that information expressing the value of a1 and a2is recorded.

With these media, the recording power suited to the linear velocity canbe determined as soon as the medium is installed in the opticalinformation recording apparatus.

The above-mentioned optical information recording medium ischaracterized in that the recording film is composed of a phase changingmaterial, and the phase changing material contains germanium andtellurium, and also contains either tin or bismuth.

With this medium, there is less incomplete erasure during overwriting inrecording at a high linear velocity, so data can be recorded at evenbetter signal quality.

The optical information recording medium of the present invention ischaracterized by having a track divided into a plurality of sectors,having embossed tracks between the sectors, and the tracks being formedsuch that the center of the embossed tracks is shifted from the centerof the recording tracks of the sectors.

With this medium, stable recording is possible even if off-trackingoccurs as a result of actuator oscillation at the boundary between arecording track and an embossed track during recording at a high linearvelocity.

To achieve the stated object, the present invention is an opticalinformation recording apparatus for irradiating an optical informationrecording medium with a laser beam, forming marks or spaces so that theoptical characteristics of a recording film are varied, forming themarks by recording pulses or a recording pulse train in which the powerof the laser beam is switched between a plurality of power levelsincluding at least a recording power and erasure power, and recordinginformation at two different linear velocities, comprising a linearvelocity setting circuit for setting two different linear velocities, arecording pulse generation circuit for generating the recording pulsesor the recording pulse train according to the setting result of thelinear velocity setting circuit, a laser drive circuit for irradiatingwith the laser beam at the plurality of power levels on the basis of therecording pulse train, and a signal quality detecting circuit fordetecting the quality of a reproduction signal, wherein the laser drivecircuit controls the recording power so as to satisfy(Pp1/Ppth1)<(Pp2/Ppth2), where Ppth1 is the threshold value of therecording power at which the quality of a reproduction signal dropsunder a specific value when a test signal is recorded at a first linearvelocity v1 with the erasure power fixed and the recording power varied,Ppth2 is the threshold value of the recording power at which the qualityof the reproduction signal drops under a specific value when the testsignal is recorded at a second linear velocity v2 that is higher thanthe first linear velocity v1, with the erasure power fixed and therecording power varied, Pp1 is the recording power when the informationis recorded at the first linear velocity v1, and Pp2 is the recordingpower when the information is recorded at the second linear velocity v2.

The present invention is an optical information recording apparatus forirradiating an optical information recording medium with a laser beam,forming marks or spaces so that the optical characteristics of arecording film are varied, forming the marks by recording pulses or arecording pulse train in which the power of the laser beam is switchedbetween a plurality of power levels including at least a recording powerand erasure power, and recording information at two different linearvelocities, comprising a linear velocity setting circuit for setting twodifferent linear velocities, a recording pulse generation circuit forgenerating the recording pulses or the recording pulse train accordingto the setting result of the linear velocity setting circuit, a laserdrive circuit for irradiating with the laser beam at the plurality ofpower levels on the basis of the recording pulse train, and a signalquality detecting circuit for detecting the quality of a reproductionsignal, wherein the laser drive circuit controls the recording power soas to satisfy (Pp1/Ppth1)<(Pp2/Ppth2), where Ppth1 is the thresholdvalue of the recording power at which the quality of a reproductionsignal drops under a specific value when a test signal is recorded at afirst linear velocity v1, with the erasure power and the recording powervaried such that the ratio between these powers is constant, Ppth2 isthe threshold value of the recording power at which the quality of thereproduction signal drops under a specific value when the test signal isrecorded at a second linear velocity v2 that is higher than the firstlinear velocity v1, with the erasure power and the recording powervaried such that the ratio between these powers is constant, Pp1 is therecording power when the information is recorded at the first linearvelocity v1, and Pp2 is the recording power when the information isrecorded at the second linear velocity v2.

The present invention is an optical information recording apparatus forirradiating an optical information recording medium with a laser beam,forming marks or spaces so that the optical characteristics of arecording film are varied, forming the marks by recording pulses or arecording pulse train in which the power of the laser beam is switchedbetween a plurality of power levels including at least a recording powerand erasure power, and recording information at two different linearvelocities, comprising a linear velocity setting circuit for setting twodifferent linear velocities, a recording pulse generation circuit forgenerating the recording pulses or the recording pulse train accordingto the setting result of the linear velocity setting circuit, a laserdrive circuit for irradiating with the laser beam at the plurality ofpower levels on the basis of the recording pulse train, and a signalquality detecting circuit for detecting the quality of a reproductionsignal, wherein the laser drive circuit controls the recording power soas to satisfy a1<a2, where a1 is the asymmetry of the reproductionsignal when a test signal is recorded at a first linear velocity v1,with the erasure power fixed and the recording power varied, and a2 isthe asymmetry of the reproduction signal when the test signal isrecorded at a second linear velocity v2 that is higher than the firstlinear velocity v1, with the erasure power fixed and the recording powervaried.

The present invention is an optical information recording apparatus forirradiating an optical information recording medium with a laser beam,forming marks or spaces so that the optical characteristics of arecording film are varied, forming the marks by recording pulses or arecording pulse train in which the power of the laser beam is switchedbetween a plurality of power levels including at least a recording powerand erasure power, and recording information at two different linearvelocities, comprising a linear velocity setting circuit for setting twodifferent linear velocities, a recording pulse generation circuit forgenerating the recording pulses or the recording pulse train accordingto the setting result of the linear velocity setting circuit, a laserdrive circuit for irradiating with the laser beam at the plurality ofpower levels on the basis of the recording pulse train, and a signalquality detecting circuit for detecting the quality of a reproductionsignal, wherein the laser drive circuit controls the recording power soas to satisfy a1<a2, where a1 is the asymmetry of the reproductionsignal when a test signal is recorded at a first linear velocity v1,with the erasure power and the recording power varied such that theratio between these powers is constant, and a2 is the asymmetry of thereproduction signal when the test signal is recorded at a second linearvelocity v2 that is higher than the first linear velocity v1, with theerasure power and the recording power varied such that the ratio betweenthese powers is constant.

With these apparatus, a mark can be formed with no distortion at lowlinear velocities, and a satisfactory power margin can be ensured inrecording at high linear velocities, so data can be recorded at goodsignal quality over a wider range of linear velocities.

With the optical information recording method of the present invention,information can be recorded at good signal quality over a wide range oflinear velocities.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a block diagram of the configuration of the recordingapparatus pertaining to a first embodiment of the present invention;

FIG. 2 is a flowchart illustrating the operation of the recordingapparatus pertaining to the first embodiment of the present invention;

FIG. 3 is a graph of jitter and recording power during low linearvelocity recording, and a diagram of the state of the recording track,in the first embodiment;

FIG. 4 is a graph of jitter and recording power during high linearvelocity recording, and a diagram of the state of the recording track,in the first embodiment;

FIG. 5 consists of graphs illustrating examples of the method forfinding the threshold value from the degree of modulation in the firstembodiment;

FIG. 6 is a block diagram of the configuration of the recordingapparatus pertaining to a second embodiment of the present invention;

FIG. 7 is a flowchart illustrating the operation of the recordingapparatus pertaining to the second embodiment of the present invention;

FIG. 8 consists of waveform diagrams and diagrams illustrating anexample of recording a mark by modulating the laser beam in low linearvelocity recording;

FIG. 9 consists of graphs of jitter and recording power in a workingexample of the present invention;

FIG. 10 consists of diagrams of the recording pulse signal, the laserirradiation waveform, and the recording state in a conventional example;

FIG. 11 is a diagram of another example of the laser irradiationwaveform in a conventional example; and

FIG. 12 is a diagram of the mark distortion during low linear velocityrecording in a conventional example.

NUMERICAL REFERENCES

-   -   1 optical disk    -   2 system control circuit    -   3 modulation circuit    -   4 recording pulse generation circuit    -   5 laser drive circuit    -   6 optical head    -   7 linear velocity setting circuit    -   8 spindle motor    -   9 reproduction signal processing circuit    -   10 jitter detecting circuit    -   11 power setting signal    -   12 modulation signal    -   13 recording pulse signal    -   14 laser beam    -   301 track    -   302 mark    -   303 molten region    -   304 wall    -   601 asymmetry detecting circuit    -   1001 leading pulse    -   1002 trailing pulse

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT

The present invention is described in more detail.

First Embodiment

First, the operation when the recording power is found by performingtest recording in the optical information recording method in the firstembodiment pertaining to the present invention will be described throughreference to FIGS. 1 to 4. The erasure power here is fixed. The qualityof the reproduction signal will be described by using jitter in thisembodiment.

FIG. 1 is a block diagram of the simplified configuration of therecording apparatus in this embodiment.

1 is an optical disk for recording or reproducing data, and 2 is asystem control circuit for controlling the overall recording apparatus.3 is a modulation circuit for generating a binarized recording datasignal according to the information to be recorded, and 4 is a recordingpulse generation circuit for generating pulses that drive a laseraccording to the recording data signal.

5 is a laser drive circuit for modulating current that drives the laserin an optical head 6 according to the pulses outputted by the recordingpulse generation circuit. The optical head 6 focuses the laser beam anddirects it at the optical disk 1. 7 is a linear velocity setting circuitfor controlling the linear velocity (that is, the rotational speed) ofthe optical disk 1, and 8 is a spindle motor for rotating the opticaldisk 1. 9 is a reproduction signal processing circuit for performingwaveform processing on a reproduction signal based on light reflectedfrom the optical disk 1, and 10 is a circuit for detecting the qualityof the reproduction signal, and more specifically, here it is a jitterdetecting circuit for obtaining a jitter value.

Next, the operation of the recording apparatus in this embodiment willbe described through reference to the flowchart of FIG. 2 and theoperational diagrams of FIGS. 3 and 4.

FIG. 2 is a flowchart illustrating the operation during test recordingin this embodiment. FIG. 3 is a graph of jitter and recording powerduring low linear velocity recording, and a diagram of the state of therecording track, in this embodiment. FIG. 4 is a graph of jitter andrecording power during high linear velocity recording, and a diagram ofthe state of the recording track.

In FIGS. 3 and 4, (a) is a graph of recording power and jitter, while(b) is the state of recording to the track when the recording power isvaried.

During recording, first, in a linear velocity setting step 201(hereinafter referred to as S201), the linear velocity setting circuit 7controls the speed of the spindle motor 8 on the basis of a command fromthe system control circuit 2, causing the optical disk 1 to rotate at aspecific linear velocity. In a seek operation step S202, the opticalhead 6 seeks a specific test recording region on the optical disk 1.

First, we will describe a test recording operation when recording at alow linear velocity v1 (that is, recording at a low transfer rate) inthis embodiment.

In a power setting step S203, the system control circuit 2 initializesthe recording power and erasure power, and sends a power setting signalto the laser drive circuit 5. These initial values may be stored aheadof time in the recording apparatus. Also, if information expressing theinitial power value has been recorded in a control track region of theoptical disk 1, the setting may be accomplished by reading thisinformation.

In a test signal recording step S204, test signal information from thesystem control circuit 2 is modulated by the modulation circuit 3. Themodulation circuit 3 modulates according to a specific modulation rule,and sends a modulation signal 12 to the recording pulse generationcircuit 4. The recording pulse generation circuit 4 sends a recordingpulse signal 13 composed of recording pulses or a recording pulse trainto the laser drive circuit 5 on the basis of the modulation signal 12.The laser drive circuit 5 modulates the power level of the laser beam14, and the laser beam 14 forms a mark corresponding to the test signalon the track.

In a recording signal reproduction step S205, the track in which thetest signal was recorded is reproduced. This reproduction signal issubjected to signal processing such as equalization or binarization bythe reproduction signal processing circuit 9.

In a jitter detecting step S206, the jitter value of the reproductionsignal that has undergone this signal processing is detected.

In a threshold value determination step S207, the system control circuit2 determines whether or not the detected jitter value is a specificthreshold value. The threshold value here is preferably near the valueat which the mark begins to be formed, rather than being near the valueat which the mark is formed sufficiently large and jitter is at itsbest. This is because the change in jitter is large with respect to thechange in recording power, so the threshold value at which the markbegins to be formed can be clearly detected, without being affected bydetection error or variance.

If the jitter value is not equal to the threshold value, then in arecording power change step S208, the recording power is changed by aspecific interval, and the flow goes back to the test signal recordingstep S204. Everything from the test signal recording step S204 throughthe recording power change step S208 is repeated until the jitter valueis sufficiently close to the threshold value.

Once the jitter value becomes sufficiently close to the threshold value,the recording power Pp1 when information is actually recorded is foundin a recording power determination step S209. To this end, first, therecording power when the jitter value has become sufficiently close tothe threshold value (this is termed Ppth1) is found. Pp1 is calculatedas follows from this value.

Pp1=Ppth1×C1

C1 here is a constant coefficient corresponding to low linear velocityrecording.

Test recording for finding the recording power is concluded at thispoint, and the recording power Pp1 thus found is used to record actualinformation to the optical disk 1.

The test recording operation when recording at a high linear velocity v2(that is, recording at a high transfer rate) in this embodiment isbasically the same as for the low linear velocity v1 discussed above.What is different from when the linear velocity is low is that thespindle motor 8 is rotated at a high linear velocity in the linearvelocity setting step S201, and that a test signal corresponding to ahigh transfer rate is recorded in the test signal recording step S204,and that in the threshold value determination step S207, the recordingpower when the jitter value has become sufficiently close to thethreshold value (this is termed Ppth2) is found, and the recording powerPp2 is calculated as follows from this value.

Pp2=Ppth2×C2

C2 here is a constant coefficient corresponding to high linear velocityrecording.

It is preferable here for the coefficient C2 during high linear velocityrecording to be greater than the coefficient C1 during low linearvelocity recording. This will be described through reference to FIGS. 3and 4.

FIGS. 3 and 4 show how jitter, the molten region, and the mark shapevary as a function of recording power when recording at the low linearvelocity v1 and the high linear velocity v2, respectively. FIGS. 3 a and4 a show the change in jitter, while FIGS. 3 b and 4 b show the changein the shape of the molten region 303 and the mark 302 on the track 301.

When recording at the low linear velocity v1, the material melts uponbeing irradiated with the laser beam, after which recrystallizationproceeds from around the edges of the molten region 303. The moltenregion 303 expands as the recording power is increased from thethreshold value Ppth1, but at the same time, the recrystallizationregion (that is, the portion left over after subtracting the mark 302from the molten region 303) also expands. Therefore, the extent to whichthe mark 302 expands as the recording power increases is less than theextent to which the molten region expands. As a result, the jitter valuealso exhibits a tendency to gradually improve (see the jitter change andthe change in recording state from point A to point B in FIG. 3).

However, if the recording power is further increased, the molten region303 will reach the walls 304 of the track. As a result, because of thefine shape of the walls 304 (causing looseness), recrystallization doesnot occur in part of the molten region reaching the walls 304, and partsof the mark 302 stick to the walls 304. This causes the jitter valuewhen the recording power has been increased to sharply deteriorate fromthat point (see the jitter change and the change in recording state frompoint B to point C in FIG. 3). Consequently, it can be seen that torecord at the low linear velocity v1 and a low jitter level, therecording power cannot be set very high with respect to the Ppth1 thatis the jitter threshold value.

On the other hand, when recording at the high linear velocity v2, sincethe relative speed between the laser spot and the medium is high, thematerial is quenched and readily enters an amorphous state after beingmelted under irradiation with the laser beam. Specifically,recrystallization does not readily proceed from the edges of the moltenregion 303, and there is little expansion of the recrystallizationregion even when the recording power is increased from the thresholdvalue Ppth2. Therefore, when the recording power is increased, the sizeof the mark 302 increases substantially in proportion to the expansionof the molten region 303. As a result, the jitter value also exhibits atendency to improve more sharply as compared to recording at the lowlinear velocity v1 (see the jitter change and the change in recordingstate from point A to point B in FIG. 4).

Since the recrystallization region does not readily expand in the caseof high linear velocity recording, the molten region 303 will not reachthe walls 304 even if the mark 302 is made larger by increasing therecording power. Accordingly, there is little worsening in jitter (seethe jitter change and the change in recording state from point B topoint C in FIG. 4).

What poses a problem in terms of recording information stably at a highlinear velocity is not so much the process of melting the recording filmand forming a mark, as it is the mechanical properties of the opticaldisk 1. As discussed above, if there is even a slight axial runout oreccentricity to the disk, the servo that moves the actuator will beunable to keep up with the axial runout or eccentricity, and defocusingor off-tracking will occur as a result. These phenomena lower theeffective power applied to the portion where the laser beam is supposedto be directed to form the mark.

In order to record stably and with little jitter even when thesephenomena occur in the course of recording at the high linear velocityv2, the recording power setting is preferably set higher than that usedat the low linear velocity v1, with respect to the Ppth1 that is thejitter threshold value. In the case of high linear velocity recording,jitter will not worsen as a result of the mark sticking to the wallseven when recording at a high recording power. Therefore, it is best torecord at an extra-high recording power so that data can be recorded atlow jitter even at an effective low power.

As discussed above, the key point of this embodiment is that the ratioof recording power to the power that is the jitter threshold value isrelatively low at low linear velocities, and is relatively large at highlinear velocities. Specifically, (Pp1/Ppth1)<(Pp2/Ppth2) is satisfied.

This minimizes the sticking of the mark to the walls in low linearvelocity recording, so the mark is formed with no distortion. Along withthis, there is an additional effect whereby stable recording is possiblewithout any worsening of jitter even if defocusing or off-trackingshould occur as a result of axial runout or eccentricity at a highlinear velocity, so information can be recorded at good signal qualityover a wider range of linear velocities.

In this embodiment, jitter in the reproduction signal was detected bythe jitter detecting circuit 10, but an error rate detecting circuit maybe provided instead of the jitter detecting circuit 10, and therecording power when information is recorded may be found from therecording power that is the error rate threshold value. With a typicalrecording apparatus, the function of detecting the error rate is handledby a circuit that demodulates information from the reproduction signal,so an advantage is that there is no need to add any special circuits.

Also, a modulation detecting circuit may be provided instead of thejitter detecting circuit 10, and the recording power when information isrecorded may be found from the recording power that is the modulationthreshold value. In addition to a method in which the absolute value ofthe degree of modulation is used as the threshold value for the degreeof modulation here, a method in which the differential coefficient of(degree of modulation/recording power) is used as the threshold valuemay be employed. Specifically, as shown in FIG. 5 a, the differentialcoefficient of (degree of modulation/recording power) αm=dm/dPp isfound. As shown in FIG. 5 b, the change in αm when the recording poweris varied is found, and the recording power at which am reaches athreshold value αth is termed Ppth1 or Ppth2. Again with this method,the threshold value can be found accurately.

Another mode in which a value based on the degree of modulation is usedas a threshold value is shown in FIG. 5 c, in which the value of (degreeof modulation×recording power) is termed β, and the β when the recordingpower is varied is found, which allows the threshold value to be foundaccurately even when the recording power at which β is the thresholdvalue βth is found at various linear velocities.

In addition to the above, as long as it is possible to find therecording power Ppth1 or Ppth2 at which a mark of a specific size beginsto be formed at various linear velocities, then any method in which athreshold value is used can be applied to the present invention.

Second Embodiment

Next, the configuration of the recording apparatus in FIG. 6 will bedescribed, as will the operation of the recording apparatus of thesecond embodiment pertaining to the present invention, through referenceto the flowchart of FIG. 7.

FIG. 6 is a block diagram of the simplified configuration of therecording apparatus in this embodiment. What is different from the firstembodiment is that an asymmetry detecting circuit 601 is providedinstead of the jitter detecting circuit 10.

FIG. 7 is a flowchart illustrating the operation during test recordingin this embodiment.

Everything from the start of the test recording up to the recordingsignal reproduction step S705 is the same as in the first embodiment.What is different is that in an asymmetry detecting step S706, theasymmetry detecting circuit 601 detects the asymmetry of thereproduction signal. How this asymmetry is found will be describedthrough reference to FIG. 8. FIGS. 8 a and 8 b show the reproductionwaveforms and the state of recording on the track when the asymmetry islarge and small, respectively. If we let IH be a high level ofreproduction signal amplitude, IL a low level, Ic a central level, andIa the average level, the asymmetry α can be found from the followingequation.

α=(Ic−Ia)/(IH−IL)

Specifically, asymmetry becomes greater as the mark becomes longer(larger).

Let us term the asymmetry at the low linear velocity v1 as the specificvalue a1, and the asymmetry at the high linear velocity v2 as thespecific value a2. The value of a2 here must be greater than that of a1.The procedure from the test recording step S704 to the recording powerchange step S708 is repeated to find the recording power at which theasymmetry is a1 at the low linear velocity v1.

In a recording power determination step S709, the recording power Pp1when information is actually recorded is the recording power at theasymmetry a1. This concludes the test recording for finding therecording power at a low linear velocity.

Similarly, in the case of the high linear velocity v2, the recordingpower Pp2 at the asymmetry a2 is found, and this power is termed therecording power when information is actually recorded.

Thus, the asymmetry of a reproduction signal is made relatively small ata low linear velocity and relatively large at a high linear velocity.Just as in the first embodiment, this minimizes the sticking of the markto the walls in low linear velocity recording, so the mark is formedwith no distortion, and stable recording is possible without anyworsening of jitter even if defocusing or off-tracking should occur as aresult of axial runout or eccentricity at a high linear velocity. Thismeans that information can be recorded at good signal quality over awider range of linear velocities.

Other Embodiments

In the above embodiments, the erasure power was fixed and the recordingpower was varied, but the same effect as above can also be achieved byobtaining a threshold value by varying erasure power and recording powerwith the ratio thereof held constant.

Also, in the above embodiments, the recording power at v1 and v2 wasdetermined by test recording, but if the respective recording powers Pp1and Pp2 at v1 and v2, or the respective coefficients C1 and C2, or therespective asymmetries a1 and a2 are prerecorded in a control track ofthe medium (that is, a region in which information related to the mediumis recorded), an advantage is that the recording power suited to thelinear velocity can be determined as soon as the medium is installed inthe optical information recording apparatus. This power levelinformation may be recorded to the medium by the optical informationrecording apparatus, or it may already have been recorded during themanufacture of the medium.

The medium in the above embodiments is preferably such that therecording film is composed of a phase changing material, and containsgermanium and tellurium, and also contains either tin or bismuth. Anadvantage in this case is that there is less incomplete erasure duringoverwriting in recording at a high linear velocity, so data can berecorded at even better signal quality.

Further, the medium in the above embodiments is preferably such that thetrack of the medium is divided into a plurality of sectors, has embossedtracks between the sectors, and the center of the embossed tracks isshifted from the center of the recording tracks of the sectors. Anadvantage in this case is that stable recording is possible even ifoff-tracking occurs as a result of actuator oscillation at the boundarybetween a recording track and an embossed track during recording at ahigh linear velocity.

The above embodiments may involve recording to a CAV recording type ofmedium.

Furthermore, the above embodiments involved two types of recording,namely, at a low linear velocity v1 and a high linear velocity v2, butwith a CAV recording system, the linear velocity and transfer ratecontinuously vary with the recording or reproduction position in themedium. In such a case, it is preferable to adopt a method in which therecording power is easily determined at an intermediate linear velocityby linking, either smoothly or in steps, the recording power at the lowlinear velocity v1 and the recording power at the high linear velocityv2. More specifically, for example, the recording power may bedetermined at an intermediate linear velocity so that the recordingpower increases along with the intermediate linear velocity.

In the above embodiments, it is preferable if the power level betweenrecording pulses is controlled to be different from the erasure power.In this case, the cooling rate during recording can be optimallycontrolled according to the linear velocity, so data can be recorded atgood signal quality.

Furthermore, in the above embodiments, the power level of the laserirradiation waveform was varied between two levels, namely, therecording power Pp and the erasure power Pb, but may instead be variedbetween three or more levels. For instance, the power level betweenrecording pulses (also called the bottom level) may be higher than Pb,or may be lower than Pb. Here, when the power coefficient betweenrecording pulses is α and α=(Pbtm−Pb)/(Pp−Pb), where Pp is the recordingpower, Pb is the erasure power, and Pbtm is the power level betweenrecording pulses, setting the power coefficient between recording pulsesso as to increase in proportion to the linear velocity is preferable inthat the cooling rate during recording at a high linear velocity willnot be excessive, and there will be little incomplete erasure duringoverwriting.

Also, the same effect as in the above embodiments will be obtained if arecording pulse train to which cooling pulses have been added is formedafter the recording pulses or recording pulse train.

Further, the above-mentioned modulation method, the length and positionof the pulses, and so forth are not limited to those given in theembodiments, and can be suitably set according to the medium and therecording conditions. Also, the edge position of the recording pulsesmay be corrected in order to avoid the effect of thermal interferencebetween marks.

Also, the above-mentioned optical disk may be made of a phase changingmaterial, an opto-magnetic material, a colorant material, or the like,any of which can be used in the present invention as long as it is amedium whose optical characteristics of the marks and spaces aredifferent from those of the spaces.

Moreover, the same effect as above can be obtained with a personalcomputer, a server, a recorder, or the like in which the opticalinformation recording method, the optical information recordingapparatus, or the optical information recording medium of the presentinvention is used.

Working Examples

More specific working examples of the first embodiment of the presentinvention will now be described.

A polycarbonate resin with a diameter of 120 mm and a thickness of 0.6mm was used for the substrate of the optical disk 1. This substrate waspreformatted by forming convex and concave pits as a control trackregion.

Information expressing the recording linear velocity for the disk wasrecorded as an identifier in the control track region. In this workingexample, the disk could be used for recording at a linear velocityranging from 24.6 to 65.6 m/s.

A recording guide groove was formed in the data region of the resinsubstrate. The guide groove had a pitch of 0.6 μm. As to the structurein which the sectors are provided within the data region, pitsexpressing address information may be formed between sectors.

Four layers comprising a protective film, a recording film, anotherprotective film, and a reflective film were formed by sputtering overthe substrate, and a protective substrate was bonded over these. Theprotective films were ZnS—SiO₂, the recording film was GeSbBiTe, and thereflective film was aluminum.

The radial position of the data region ranged from 21.9 to 58.4 mm, andtest recording regions were provided at two locations, namely, on theinside and outside of the data region. Specifically, the radial positionof the test recording regions ranged from 21.8 to 21.9 mm and from 58.4to 58.5 mm.

When this disk was rotated at a constant speed of 10,727 rpm (that is,equal rotation speed), recording or reproduction was performed at alinear velocity of 24.6 m/s at the innermost part of the data region(that is, at a radius of 21.9 mm), and at a linear velocity of 65.6 m/sat the outermost part (that is, at a radius of 58.4 mm).

With a CAV recording system, recording is performed with the lineardensity held constant by varying the channel clock period according tothe change in linear velocity from the inner to outer periphery. In thisworking example, the information modulation system was (8-16) pulsewidth modulation, and the channel clock period was set so that theshortest mark length would be 0.40 μm.

First, the disk was rotated at a linear velocity of 24.6 m/s, the focusand tracking servos were actuated, and the focus error signal wasobserved, but no pronounced fluctuation was seen. The maximum residualerror of the focus error signal was measured and converted into theamount of movement in the optical axis direction of the actuator, whichgave a result of 0.1 μm (zero-peak amplitude).

The disk was then rotated at 65.6 m/s, whereupon there were localinstances of spiking of the focus error signal. The maximum residualerror of the local spiking was 1.2 μm. The length of this local spikingwas approximately one-tenth of a rotation in the track direction, nopronounced fluctuations were seen anywhere else, and the maximumresidual error was 0.2 μm.

A place on the disk where there was no spiking of the focus error signalremainder was selected, and the relation between recording power andjitter was measured at a minimum linear velocity of 24.6 ml/s and amaximum linear velocity of 65.6 m/s, with the erasure power fixed andthe recording power varied. The erasure power here was 8 mW at 24.6 m/s,and 11 mW at 65.6 m/s.

These measurement results are given in FIG. 9. FIG. 9 a shows theresults of measurement at a linear velocity of 24.6 s/m, and FIG. 9 bshows the results of measurement at a linear velocity of 65.6 m/s. If weassume the jitter threshold value to be 13%, the recording power atwhich the threshold value is attained was 14 mW at 24.6 ml/s and 21 mWat 65.6 m/s. The recording power jitter when the coefficient C1 or C2was 1.2, the recording power when the coefficient was 1.3, and thejitter were found on the basis of these power levels, the results ofwhich are given in Tables 1 and 2.

TABLE 1 linear velocity: 24.6 m/s Recording power (mW) Jitter (%) C1 =1.2 16.8 9.2 C1 = 1.3 18.2 10.5

TABLE 2 linear velocity: 65.6 m/s Recording power (mW) Jitter (%) C2 =1.2 25.2 9.1 C2 = 1.3 27.3 9.4

It can be seen from these tables that jitter worsens sharply at C1=1.3as compared to when C1=1.2 at a linear velocity of 24.6 m/s. Meanwhile,at a linear velocity of 65.6 m/s, there was little worsening in jitterwhen C2 was raised from 1.2 to 1.3.

Next, only a place where there was no spiking of the focus error signalwas selected, and the jitter was measured when data was recorded atrecording power levels of C2=1.2 and 1.3. These results are given inTable 3. FIG. 9 c shows the results of measuring the relation betweenrecording power and jitter.

TABLE 3 linear velocity: 65.6 m/s Recording power (mW) Jitter (%) C2 =1.2 25.2 11.2 C2 = 1.3 27.3 9.4

The jitter above was the same as in Table 2 when C2=1.3, but was worsewhen C2=1.2. The reproduction signal of the track recorded at C2=1.2 wasobserved, and the signal amplitude had decreased at the same placeswhere the focus error signal was locally spiked. This seems to indicatethat jitter worsened at C2=1.2, at which there was no margin for errorwhen the power was decreased, because there was an effective decrease inthe irradiation energy at the places where defocusing had occurredlocally.

It can be seen from the above that with this disk, stable recording atlow jitter can be performed, at either the lowest or the highest linearvelocity, by setting C1 to 1.2 at a linear velocity of 24.6 m/s and C2to 1.3 at a linear velocity of 65.6 m/s (that is, setting to C1<C2).

Also, the reproduction signal of this disk was demodulated and the biterror rate of the data was measured. The correlation between jitter andthe bit error rate was found, which revealed that no bit error occurredwhen the jitter was 9.5% or lower.

This tells us that reproduction at higher quality is possible within theC1 and C2 ranges, in which jitter is 9.5% or less, so these ranges arepreferable. The results in FIG. 9 a indicate that these ranges are1.14≦C1≦1.24 at a linear velocity of 24.6 m/s, and 1.25≦C2≦1.33 at alinear velocity of 65.6 m/s.

INDUSTRIAL APPLICABILITY

The optical information recording method, optical information recordingapparatus, and optical information recording medium of the presentinvention can also be applied to a personal computer, a server, arecorder, or the like, and the same effect as above can be obtained.

1-27. (canceled)
 28. An optical information recording method comprising,irradiating an optical information recording medium with a laser beam,forming marks or spaces so that the optical characteristics of arecording film are varied, forming the marks by recording pulses or arecording pulse train in which the power of the laser beam is switchedbetween a plurality of power levels including at least a recording powerand erasure power, and recording information at two different linearvelocities, wherein the recording power is controlled so as to satisfy(Pp1/Ppth1)<(Pp2/Ppth2), where Ppth1 is the threshold value of therecording power at which the quality of a reproduction signal dropsunder a specific value when a test signal is recorded at a first linearvelocity v1 with the erasure power fixed and the recording power varied,Ppth2 is the threshold value of the recording power at which the qualityof the reproduction signal drops under a specific value when the testsignal is recorded at a second linear velocity v2 that is higher thanthe first linear velocity v1, with the erasure power fixed and therecording power varied, Pp1 is the recording power when the informationis recorded at the first linear velocity v1, and Pp2 is the recordingpower when the information is recorded at the second linear velocity v2.29. The optical information recording method according to claim 28,wherein the criterion for the quality of the reproduction signal is thejitter of the reproduction signal.
 30. The optical information recordingmethod according to claim 28, wherein the criterion for the quality ofthe reproduction signal is a value based on the error rate of thereproduction signal.
 31. The optical information recording methodaccording to claim 28, wherein the criterion for the quality of thereproduction signal is a value based on the degree of modulation of thereproduction signal.
 32. An optical information recording methodcomprising, irradiating an optical information recording medium with alaser beam, forming marks or spaces so that the optical characteristicsof a recording film are varied, forming the marks by recording pulses ora recording pulse train in which the power of the laser beam is switchedbetween a plurality of power levels including at least a recording powerand erasure power, and recording information at two different linearvelocities, wherein the recording power is controlled so as to satisfy(Pp1/Ppth1)<(Pp2/Ppth2), where Ppth1 is the threshold value of therecording power at which the quality of a reproduction signal dropsunder a specific value when a test signal is recorded at a first linearvelocity v1, with the erasure power and the recording power varied suchthat the ratio between these powers is constant, Ppth2 is the thresholdvalue of the recording power at which the quality of the reproductionsignal drops under a specific value when the test signal is recorded ata second linear velocity v2 that is higher than the first linearvelocity v1, with the erasure power and the recording power varied suchthat the ratio between these powers is constant, Pp1 is the recordingpower when the information is recorded at the first linear velocity v1,and Pp2 is the recording power when the information is recorded at thesecond linear velocity v2.
 33. An optical information recording methodcomprising, irradiating an optical information recording medium with alaser beam, forming marks or spaces so that the optical characteristicsof a recording film are varied, forming the marks by recording pulses ora recording pulse train in which the power of the laser beam is switchedbetween a plurality of power levels including at least a recording powerand erasure power, and recording information at two different linearvelocities, wherein the recording power is controlled so as to satisfya1<a2, where a1 is the asymmetry of the reproduction signal when a testsignal is recorded at a first linear velocity v1, with the erasure powerfixed and the recording power varied, and a2 is the asymmetry of thereproduction signal when the test signal is recorded at a second linearvelocity v2 that is higher than the first linear velocity v1, with theerasure power fixed and the recording power varied.
 34. An opticalinformation recording method comprising, irradiating an opticalinformation recording medium with a laser beam, forming marks or spacesso that the optical characteristics of a recording film are varied,forming the marks by recording pulses or a recording pulse train inwhich the power of the laser beam is switched between a plurality ofpower levels including at least a recording power and erasure power, andrecording information at two different linear velocities, wherein therecording power is controlled so as to satisfy a1<a2, where a1 is theasymmetry of the reproduction signal when a test signal is recorded at afirst linear velocity v1, with the erasure power and the recording powervaried such that the ratio between these powers is constant, and a2 isthe asymmetry of the reproduction signal when the test signal isrecorded at a second linear velocity v2 that is higher than the firstlinear velocity v1, with the erasure power and the recording powervaried such that the ratio between these powers is constant.
 35. Theoptical information recording method according to claim 28, wherein therecording system is a CAV recording system.
 36. The optical informationrecording method according to claim 28, wherein the recording power iscontrolled so that Pp is increased according to the increase in a linearvelocity v when Pp is the recording power at the linear velocity v,which is a value between the first linear velocity v1 and the secondlinear velocity v2.
 37. The optical information recording methodaccording to claim 28, wherein the power level between recording pulsesis controlled to be different from the erasure power.
 38. The opticalinformation recording method according to claim 28, wherein the powercoefficient between recording pulses at the second linear velocity v2 iscontrolled to be higher than the power coefficient between recordingpulses at the first linear velocity v1 when the power coefficientbetween recording pulses is α and α=(Pbtm−Pb)/(Pp−Pb), where Pp is therecording power, Pb is the erasure power, and Pbtm is the power levelbetween recording pulses.
 39. The optical information recording methodaccording to claim 33, wherein the recording power is controlled so thatPp is increased according to the increase in a linear velocity v when Ppis the recording power at the linear velocity v, which is a valuebetween the first linear velocity v1 and the second linear velocity v2.40. The optical information recording method according to claim 33,wherein the power level between recording pulses is controlled to bedifferent from the erasure power.
 41. The optical information recordingmethod according to claim 33, wherein the power coefficient betweenrecording pulses at the second linear velocity v2 is controlled to behigher than the power coefficient between recording pulses at the firstlinear velocity v1 when the power coefficient between recording pulsesis α and α=(Pbtm−Pb)/(Pp−Pb), where Pp is the recording power, Pb is theerasure power, and Pbtm is the power level between recording pulses. 42.An optical information recording medium with which information isrecorded by the method according to claim 28, wherein informationexpressing the value of Pp1/Ppth1 and Pp2/Ppth2 is recorded.
 43. Anoptical information recording medium with which information is recordedby the method according to claim 32, wherein information expressing thevalue of Pp1/Ppth1 and Pp2/Ppth2 is recorded.
 44. An optical informationrecording medium with which information is recorded by the methodaccording to claim 28, wherein information expressing the value of Pp1and Pp2 is recorded.
 45. An optical information recording medium withwhich information is recorded by the method according to claim 32,wherein information expressing the value of Pp1 and Pp2 is recorded. 46.An optical information recording medium with which information isrecorded by the method according to claim 33, wherein informationexpressing the value of a1 and a2 is recorded.
 47. An opticalinformation recording medium with which information is recorded by themethod according to claim 34, wherein information expressing the valueof a1 and a2 is recorded.
 48. The optical information recording mediumaccording to claim 42, wherein the recording film is composed of a phasechanging material, and the phase changing material contains germaniumand tellurium, and also contains either tin or bismuth.
 49. The opticalinformation recording medium according to claim 44, wherein therecording film is composed of a phase changing material, and the phasechanging material contains germanium and tellurium, and also containseither tin or bismuth.
 50. The optical information recording mediumaccording to claim 46, wherein the recording film is composed of a phasechanging material, and the phase changing material contains germaniumand tellurium, and also contains either tin or bismuth.
 51. The opticalinformation recording medium according to claim 42, having a trackdivided into a plurality of sectors, having embossed tracks between thesectors, and the tracks being formed such that the center of theembossed tracks is shifted from the center of the recording tracks ofthe sectors.
 52. The optical information recording medium according toclaim 44, having a track divided into a plurality of sectors, havingembossed tracks between the sectors, and the tracks being formed suchthat the center of the embossed tracks is shifted from the center of therecording tracks of the sectors.
 53. The optical information recordingmedium according to claim 46, having a track divided into a plurality ofsectors, having embossed tracks between the sectors, and the tracksbeing formed such that the center of the embossed tracks is shifted fromthe center of the recording tracks of the sectors.
 54. The opticalinformation recording medium according to claim 48, having a trackdivided into a plurality of sectors, having embossed tracks between thesectors, and the tracks being formed such that the center of theembossed tracks is shifted from the center of the recording tracks ofthe sectors.
 55. An optical information recording apparatus forirradiating an optical information recording medium with a laser beam,forming marks or spaces so that the optical characteristics of arecording film are varied, forming the marks by recording pulses or arecording pulse train in which the power of the laser beam is switchedbetween a plurality of power levels including at least a recording powerand erasure power, and recording information at two different linearvelocities, comprising: a linear velocity setting circuit for settingtwo different linear velocities; a recording pulse generation circuitfor generating the recording pulses or the recording pulse trainaccording to the setting result of the linear velocity setting circuit;a laser drive circuit for irradiating with the laser beam at theplurality of power levels on the basis of the recording pulse train; anda signal quality detecting circuit for detecting the quality of areproduction signal, wherein the laser drive circuit controls therecording power so as to satisfy (Pp1/Ppth1)<(Pp2/Ppth2), where Ppth1 isthe threshold value of the recording power at which the quality of areproduction signal drops under a specific value when a test signal isrecorded at a first linear velocity v1 with the erasure power fixed andthe recording power varied, Ppth2 is the threshold value of therecording power at which the quality of the reproduction signal dropsunder a specific value when the test signal is recorded at a secondlinear velocity v2 that is higher than the first linear velocity v1,with the erasure power fixed and the recording power varied, Pp1 is therecording power when the information is recorded at the first linearvelocity v1, and Pp2 is the recording power when the information isrecorded at the second linear velocity v2.
 56. The optical informationrecording apparatus according to claim 55, wherein the signal qualitydetecting circuit is a jitter detecting circuit that detects jitter in areproduction signal.
 57. The optical information recording apparatusaccording to claim 55, wherein the signal quality detecting circuit isan error rate detecting circuit that detects the error rate of areproduction signal.
 58. The optical information recording apparatusaccording to claim 55, wherein the signal quality detecting circuit is amodulation detecting circuit that detects the degree of modulation in areproduction signal.
 59. An optical information recording apparatus forirradiating an optical information recording medium with a laser beam,forming marks or spaces so that the optical characteristics of arecording film are varied, forming the marks by recording pulses or arecording pulse train in which the power of the laser beam is switchedbetween a plurality of power levels including at least a recording powerand erasure power, and recording information at two different linearvelocities, comprising: a linear velocity setting circuit for settingtwo different linear velocities; a recording pulse generation circuitfor generating the recording pulses or the recording pulse trainaccording to the setting result of the linear velocity setting circuit;a laser drive circuit for irradiating with the laser beam at theplurality of power levels on the basis of the recording pulse train; anda signal quality detecting circuit for detecting the quality of areproduction signal, wherein the laser drive circuit controls therecording power so as to satisfy (Pp1/Ppth1)<(Pp2/Ppth2), where Ppth1 isthe threshold value of the recording power at which the quality of areproduction signal drops under a specific value when a test signal isrecorded at a first linear velocity v1, with the erasure power and therecording power varied such that the ratio between these powers isconstant, Ppth2 is the threshold value of the recording power at whichthe quality of the reproduction signal drops under a specific value whenthe test signal is recorded at a second linear velocity v2 that ishigher than the first linear velocity v1, with the erasure power and therecording power varied such that the ratio between these powers isconstant, Pp1 is the recording power when the information is recorded atthe first linear velocity v1, and Pp2 is the recording power when theinformation is recorded at the second linear velocity v2.
 60. An opticalinformation recording apparatus for irradiating an optical informationrecording medium with a laser beam, forming marks or spaces so that theoptical characteristics of a recording film are varied, forming themarks by recording pulses or a recording pulse train in which the powerof the laser beam is switched between a plurality of power levelsincluding at least a recording power and erasure power, and recordinginformation at two different linear velocities, comprising: a linearvelocity setting circuit for setting two different linear velocities; arecording pulse generation circuit for generating the recording pulsesor the recording pulse train according to the setting result of thelinear velocity setting circuit; a laser drive circuit for irradiatingwith the laser beam at the plurality of power levels on the basis of therecording pulse train; and a signal quality detecting circuit fordetecting the quality of a reproduction signal, wherein the laser drivecircuit controls the recording power so as to satisfy a1<a2, where a1 isthe asymmetry of the reproduction signal when a test signal is recordedat a first linear velocity v1, with the erasure power fixed and therecording power varied, and a2 is the asymmetry of the reproductionsignal when the test signal is recorded at a second linear velocity v2that is higher than the first linear velocity v1, with the erasure powerfixed and the recording power varied.
 61. An optical informationrecording apparatus for irradiating an optical information recordingmedium with a laser beam, forming marks or spaces so that the opticalcharacteristics of a recording film are varied, forming the marks byrecording pulses or a recording pulse train in which the power of thelaser beam is switched between a plurality of power levels including atleast a recording power and erasure power, and recording information attwo different linear velocities, comprising: a linear velocity settingcircuit for setting two different linear velocities; a recording pulsegeneration circuit for generating the recording pulses or the recordingpulse train according to the setting result of the linear velocitysetting circuit; a laser drive circuit for irradiating with the laserbeam at the plurality of power levels on the basis of the recordingpulse train; and a signal quality detecting circuit for detecting thequality of a reproduction signal, wherein the laser drive circuitcontrols the recording power so as to satisfy a1<a2, where a1 is theasymmetry of the reproduction signal when a test signal is recorded at afirst linear velocity v1, with the erasure power and the recording powervaried such that the ratio between these powers is constant, and a2 isthe asymmetry of the reproduction signal when the test signal isrecorded at a second linear velocity v2 that is higher than the firstlinear velocity v1, with the erasure power and the recording powervaried such that the ratio between these powers is constant.
 62. Theoptical information recording apparatus according to claim 55, whereinthe recording system is a CAV recording system.
 63. The opticalinformation recording apparatus according to claim 55, wherein therecording power is controlled so that Pp is increased according to theincrease in a linear velocity v when Pp is the recording power at thelinear velocity v, which is a value between the first linear velocity v1and the second linear velocity v2.
 64. The optical information recordingapparatus according to claim 60, wherein the recording power iscontrolled so that Pp is increased according to the increase in a linearvelocity v when Pp is the recording power at the linear velocity v,which is a value between the first linear velocity v1 and the secondlinear velocity v2.
 65. The optical information recording apparatusaccording to claim 55, wherein the power level between recording pulsesis controlled to be different from the erasure power.
 66. The opticalinformation recording apparatus according to claim 60, wherein the powerlevel between recording pulses is controlled to be different from theerasure power.
 67. The optical information recording apparatus accordingto claim 55, wherein the power coefficient between recording pulses atthe second linear velocity v2 is controlled to be higher than the powercoefficient between recording pulses at the first linear velocity v1when the power coefficient between recording pulses is α andα=(Pbtm−Pb)/(Pp−Pb), where Pp is the recording power, Pb is the erasurepower, and Pbtm is the power level between recording pulses.
 68. Theoptical information recording apparatus according to claim 60, whereinthe power coefficient between recording pulses at the second linearvelocity v2 is controlled to be higher than the power coefficientbetween recording pulses at the first linear velocity v1 when the powercoefficient between recording pulses is α and α=(Pbtm−Pb)/(Pp−Pb), wherePp is the recording power, Pb is the erasure power, and Pbtm is thepower level between recording pulses.